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  • - [Instructor] So here's a question.

  • If you got two positive charges,

  • we know they're gonna repel.

  • So if I put these next to each other,

  • this blue charge would repel

  • the green charge and vice versa,

  • but how is that working exactly?

  • I mean there's nothing in between these charges.

  • How is the blue charge pushing on the green charge

  • when it's not even touching it?

  • So this is kind of a weird thing, right?

  • If I want to push on something in my room,

  • I need to walk up to that thing

  • and actually physically touch it,

  • and then give it a shove.

  • Yet this blue charge seemingly exerts a force

  • on the green charge with just empty space in between, right?

  • There's no strings here.

  • What is the mechanism?

  • So physicists were kind of embarrassed

  • and concerned about this.

  • So it was like, all right, we can calculate exactly

  • how much force there would be on each charge

  • but we don't really know how that is actually working.

  • It doesn't seem to be making any sense

  • that a charge can push on another charge

  • across potentially vast stretches of the universe here.

  • This could be a huge distance

  • and yet somehow this charge over here knows,

  • ah, there's a charge over here pushing on me.

  • How is that possible?

  • This isn't new to electrical forces.

  • This was a problem when Newton came up

  • with the force of gravity.

  • When Newton figured out how to calculate

  • the force of gravity, he showed, okay,

  • we can calculate how much the earth is gonna pull

  • on the moon and people were like,

  • this is great because now we can calculate

  • and predict the orbits of the planets and comets.

  • But when people were like, hey, Newton, that's really cool,

  • but how is the earth pulling on the moon

  • when there's nothing in between?

  • Newton was basically like I don't know exactly

  • why that works but I know the math

  • lets me predict it exactly.

  • And so ever since the time of Newton,

  • this has been kind of in the back of physicists' minds

  • for hundreds of years now

  • as we let up to the electric force.

  • People were kind of like, all right,

  • how was this force at a distance actually being transmitted?

  • Is there something in between here

  • that's actually letting the earth pull on the moon?

  • So finally when people were dealing

  • with this electrical phenomenon,

  • they decided, all right, it's time,

  • it's time to answer how the two objects

  • exert forces on each other

  • across what a potentially vast distances of space.

  • The person who came up with an explanation

  • was named Michael Faraday.

  • So this is Michael Faraday right here.

  • He did his science in the 1800s generally regarded

  • as one of the most important physicist/chemist

  • of all time really.

  • What Faraday said is this, he said,

  • guys, here's how it's working.

  • So this positive charge over here.

  • So forget about the other positive.

  • Forget about this green positive for a minute.

  • Let's just focus on this blue one.

  • He said, here's what the blue charge is really doing.

  • He said this blue charge is creating

  • an electric field all around it

  • and we'll abbreviate this electric field with a capital E.

  • Since it's a vector,

  • we'll put a little vector arrow over the top.

  • So Faraday said this positive charge creates

  • an electric field everywhere around it at all times

  • whether there's other charges nearby or not.

  • The electric field gets weaker and weaker

  • the farther out you go.

  • So near the charge you've got a big electric field

  • and then the farther away you go,

  • the weaker the electric field is.

  • So this is kind of like a spider web surrounding a spider

  • except the spider is like the charge

  • and the web is like the electric field.

  • Now you gotta be careful.

  • People see this and they think oh,

  • this is just like electric force, right?

  • But this is not a force.

  • These vectors here are not forces.

  • This is where people get really mixed up.

  • They look like forces because people are like

  • we use arrows to draw forces before.

  • Aren't these just forces?

  • They're not.

  • It's a vector so we represent them with arrows

  • but the electric field is

  • not the exact same thing as electric force.

  • So you gotta keep that straight.

  • They are not the same thing.

  • They're very related but they are not the same thing.

  • Electric force is F.

  • We represent it with F

  • and maybe a little e for electric force

  • and since it's a vector

  • maybe we can draw it with a vector sign.

  • But the electric force is

  • not the same thing as electric field E.

  • How are they related?

  • Here's how it works.

  • So even though the electric field is not a force,

  • it can cause an electric force on other charges.

  • So as it stands right now,

  • if all we had was a positive charge,

  • creating its electric field in the region surrounding it,

  • there would be no electric force.

  • You need two charges to have an electrical force.

  • This charge is not gonna exert a force on itself.

  • This blue charge and they keep these all straight.

  • Let's just give this a name.

  • We'll call this Q one.

  • This charge Q one creates an electric field

  • but that electric field, I'll call it E one

  • because it's created by Q one.

  • This E one does not exert a force on Q one.

  • It will exert a force on any other charges

  • that wander into this region.

  • So this electric field that gets created by Q one

  • just sits and waits patiently

  • just like a spider web waits around the spider

  • for another charge to wander in.

  • Then it will exert a force on it.

  • Let's put another charge in here.

  • Let's say this positive charge has wandered into this zone

  • for some reason who knows why.

  • If it wanders into this region,

  • there will be an electric force on this charge.

  • Here's the story that Michael Faraday told us

  • that made us feel better

  • about how this force at a distance works.

  • Michael Faraday said, "Here's what's really happening.

  • "This positive charge Q one is creating an electric field

  • "all around it including this point over here

  • "where Q two is."

  • So we'll call this charge Q two.

  • So there was already an electric field at that point

  • that was being created by Q one.

  • Now, when this Q two wanders into this region,

  • the Q two just has to look at its immediate surroundings.

  • At this point right here it sees this electric field.

  • It senses it and it knows,

  • okay, an electric field pointing to the right.

  • That's gonna cause a force on me to the right.

  • So it causes an electric force.

  • The electric field is not an electric force

  • but it will cause an electric force on a charge

  • that wanders around into it.

  • You might wander how is this any better.

  • Well it keep things local.

  • So physicists like it when things stay

  • what we call a local.

  • By local, we mean, okay, this charge Q two.

  • In order to figure out what it should do,

  • all it has to know about is the things

  • and the space immediately surrounding it.

  • So it just samples the electric field

  • that at this point right here,

  • it says, oh, there's an electric field pointing this way.

  • I'm gonna feel an electric force into that direction.

  • In other words, it doesn't have to know.

  • It doesn't have to say, oh there's this positive charge

  • on this other side of the galaxy

  • and that's the thing exerting a force on me.

  • Nope, it just knows.

  • Oh, there's an electric field right here.

  • That's all I need to know to figure out

  • the electric force on me.

  • So that's sort of how Faraday got around this question

  • of how does one object exert a force on another object

  • when there's nothing in between.

  • He said there's a mediator basically

  • that this first charge creates a field everywhere

  • including at this point

  • and then that field is creating a force on this charge

  • that wanders into that zone.

  • So yes, conceptually the way you could think

  • about it is this.

  • This charge Q one is creating the electric field E one.

  • This electric field in this region is causing a force

  • on this charge Q two

  • and that's how Q two knows to feel the force

  • it's supposed to feel which keeps things local.

  • This Q two just has to know about the field right

  • in its vicinity in order to figure out what to do.

  • It doesn't have to know about things

  • on the other side of the universe.

  • But you could complain at this point.

  • You might be like, "Wait a minute.

  • "Doesn't Q two also create its own electric field?

  • "Wouldn't Q two also create an electric field

  • "every where around it?"

  • We could call that E two

  • since it's created by charge too.

  • Doesn't it create its own electric field

  • just like all charges do?

  • Yeah, it does.

  • In fact it will create an electric field over here

  • next to Q one and that's how Q one knows

  • it's supposed to feel the force it feels

  • in the direction that it feels it.

  • So that's how these charges talk to each other.

  • You could think about it that way.

  • The way charges talk to each other

  • is with the electric field.

  • One charge creates an electric field

  • over by the other charge.

  • That charge feels the force.

  • The other charge creates a field by the first charge.

  • That first charge feels the force.

  • So conceptually that's how this electric field works

  • and that's how it does.

  • So at this point you might not be impressed.

  • You might be like, "Are we just making up a story

  • "to make ourselves feel better here?

  • "Is this just some elaborate fairy tale that makes us

  • "so that we don't feel so awkward

  • "talking about things exerting forces

  • "on each other at a distance?

  • "Is there any benefit for doing this?"

  • And there is, there's a big benefit.

  • Mathematically in terms of physics,

  • talking about the electric field

  • makes describing the physics way easier.

  • In fact it makes it so that you don't even have to know

  • about the charge creating that field at all.

  • If you have a way of knowing the field

  • even if you don't know what charge is creating that fied,

  • you could figure out what the force is gonna be

  • on any charge in that field without even knowing

  • the charge that created that field

  • and that turns out to happen a lot.

  • So knowing the electric field is extremely useful.

  • It lets you determine the electric force on a charge

  • even if you don't know what charge is exerting that force.

  • So up to this point, I've been trying to motivate

  • why we would want this idea of the electric field,

  • why physicists would come up with this idea.

  • But I wouldn't blame you if at this point

  • you aren't thinking, I still don't know

  • what electric field is.

  • I know what it isn't.

  • Electric field is not electric force

  • but what exactly is the electric field.

  • So let me give the electric field a proper definition here.

  • The electric field E at a point in space

  • is defined to be the amount of electric force

  • per charge exerted at that point in space.

  • So this is what the electric field is.

  • It's the force per charge.

  • The way physicists usually think about this is

  • imagine throwing a test charge in here.

  • We call this a test charge.

  • We'd like to imagine that this charge is really little

  • so that it doesn't completely likes swamped and overwhelmed.

  • The other charge is creating this field.

  • Otherwise if you threw some huge charge in here,

  • all the other charge would scatter

  • and it would change the whole situation.

  • So let's say we put a really small test charge in here.

  • If I want to know what the electric field is at a point

  • in space, I'd just bring my test charge over here,

  • measure the amount of electric force on that test charge

  • and then I just divide by how much was there

  • in that test charge.

  • What was the charge of that test charge?

  • I'll call this charge two.

  • If I take the force on charge two,

  • divide it by charge two,

  • that would be the value of the electric field

  • at that point in space.

  • So this is how we define the electric field.

  • The definition of electric field is

  • the amount of force per charge.

  • In other words, let's put some numbers in here.

  • Let's say Q two was two coulombs.

  • This is actually an enormous amount of charge.

  • This is kind of unrealistic example

  • but it will make the numbers come out nice

  • and conceptually it's the same thing.

  • So a positive two coulombs was placed here.

  • That's the value of Q two.

  • Let's say when we measure the force on Q two,

  • we're getting 10 newtons of force.

  • In that case, we can just say,

  • "All right, then the electric field,

  • "in that region of that vicinity

  • "is gonna be 10 newtons of force per two coulombs of charge

  • "and we get an electric field of five.

  • "Then the units are newtons per coulomb."

  • And that makes sense because what the electric field

  • is really telling you is how many newtons of force

  • you would get per coulomb.

  • If you put more coulombs at that point in space,

  • there'd be a greater force.

  • This number is telling you the number of newtons

  • you would get per coulomb.

  • Since we had two coulombs at this point in space

  • and there was five newtons per coulomb,

  • the force was 10 newtons.

  • So this number five newtons per coulomb is important

  • because it's the same for any charge you put there.

  • This is why the electric field is useful.

  • At this point in space right here,

  • if the electric field is five,

  • it's five newtons per coulomb

  • no matter what charge you put there.

  • So if I put a four coulombs charge at that point,

  • since there's five newtons for every coulomb,

  • there'd be a 20 newton force there

  • because there's five newtons for every coulomb.

  • If there's four coulombs, there'd be five times four newtons

  • which is 20 newtons.

  • So you can imagine rearranging this formula another way.

  • You could just multiply those sides by Q

  • and you get that the electric force on a charge

  • is equal to the value of that charge at that point in space

  • multiplied by the value of the electric field

  • at that point in space.

  • But it's important to note this electric field is

  • not created by this charge Q two.

  • This was created by some other charge

  • or collection of charges.

  • Remember this charge Q one is creating this electric field

  • E one and that electric field is causing

  • this electric force on Q two.

  • Q two did not create the electric field E one

  • that it interacted with.

  • Q one created that electric field E one.

  • So people get mixed up.

  • They see this formula.

  • They start to think

  • maybe this Q two is creating this electric field.

  • It's not.

  • This electric field is causing the electric force

  • on that charge, not the other way around.

  • This Q two is not creating this field.

  • This field is causing the force on that charge.

  • So this formula is extremely useful.

  • If you know the electric field at a point in space,

  • you can figure out the electric force on any charge

  • at that point by just multiplying the two values together

  • to get the electric force.

  • So you can see now that the electric field

  • is not the electric force.

  • It's the amount of electric force per charge

  • at a point in space.

  • Very related but different.

  • Different enough that you have to keep these ideas separate.

  • Electric field is not electric force, and vice versa.

  • Electric force is not electric field.

  • The electric field is the amount

  • of electric force per charge

  • and the electric force on a charge at some point in space

  • is the amount of charge times the electric field

  • at that point in space.

  • So recapping, electric charges create electric fields.

  • These electric fields enter and cause forces

  • on charges that exists in that region.

  • The value of the electric field is representing

  • the number of newtons of force per coulomb

  • at that point in space.

  • In terms of a formula, the electric field

  • is the amount of force per charge

  • or in other words the amount of electric force

  • is the charge times the electric field

  • at that point in space.

- [Instructor] So here's a question.

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A2 初級 美國腔

02-1(Electric field definition | Electric charge, field, and potential | Physics | Khan Academy)

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    yukang920108 發佈於 2022 年 07 月 19 日
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